One may ask what the first hints would be in collider
data from beyond the SM effects of the \(B_3-L_2\)  model. The
answer, possibly, is the \(b \rightarrow s \mu ^+ \mu ^-\)  anomalies that are currently being
investigated [1]}, [2]}, [3]}. One can
also obtain deviations in \(M_W\) , as figure REF 
implies. This figure also reminds us that (since we have applied the current
bounds, the sensitivity of which will increase with increased integrated
luminosity) the LHC may also observe deviations
from the SM limit in the signal strength of various Higgs
cross-sections, should the flavon and Higgs fields mix. The first direct
evidence for the model, however, would
likely be from the classic \(Z^\prime \rightarrow \mu ^+ \mu ^-\) 
resonance search, followed possibly by other \(Z^\prime \)  decay modes.
Flavon particle production (via the usual Higgs production modes, but
suppressed by
powers of \(\sin \phi \) ) could also be observed.
Flavonstrahlung may
eventually be observed at future colliders, with a resonant \(\mu ^+ \mu ^-\) 
produced in association with a
flavon boson, which would primarily
decay to \(W^+W^-\) , \(ZZ\)  or \(HH\) , as
displayed on figure REF .
